Question 5 of 5: Transient Drawdown Near a River (Constant-Head) and Near an Impermeable Boundary
Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)
Notes on this paper
National Exams — December 2015 — 04-Geol-A2 Hydrogeology. Three-hour, open-book exam; any non-communicating calculator permitted. Five questions constitute a complete paper and all five are of equal value; most call for an essay-format answer with clarity and organization counted. Unless stated otherwise, water density is taken as 1000 kg/m³, water viscosity as 0.001 kg/m-sec, and g as 9.81 m/s².
Reference texts: Freeze & Cherry, Groundwater (Prentice-Hall, 1979) — Darcy's law, soil phase relations, the Theis and Thiem well equations, leaky-aquifer (Hantush-Jacob) theory, image-well boundary methods, and density-dependent flow; Todd & Mays, Groundwater Hydrology — unconfined-well hydraulics and Dupuit-Forchheimer flow; EGBC Geoscience Professional Practice Guidelines for assumption-disclosure conventions on open-book calculations.
Question 5: Transient Drawdown Near a River (Constant-Head) and Near an Impermeable Boundary (equal value)
Given. Confined aquifer, thickness $b=30$ m, $S_s=2.3\times10^{-5}\ \text{m}^{-1}$, $K=1.2\times10^{-5}$ m/s. Pumping rate $Q=50\ \text{m}^3/\text{hr}=0.01389\ \text{m}^3/\text{s}$. Pumping well 200 m west of a linear boundary. (a) Constant-head (river) boundary; observation well 60 m south of the pumping well; $t=24$ and 36 h. (b) Impermeable boundary instead; observation well 200 m south of the pumping well; $t=36$ h.
Find. Drawdown at each observation well/time using the method of images.
Approach. First compute the aquifer's $T=Kb$ and $S=S_sb$. A constant-head boundary is modelled by an image RECHARGE well (equal $-Q$) mirrored across the boundary, so the total drawdown is the real well's Theis drawdown minus the image well's; an impermeable (no-flow) boundary is modelled by an image PUMPING well (equal $+Q$) at the same mirror location, so the two drawdowns simply add. Place the pumping well at the origin with the boundary running north–south 200 m to the west; the image well sits a further 200 m west of the boundary, i.e. 400 m due west of the pumping well.
Part (a) — distances to the real and image wells. With the pumping well at $(0,0)$, the observation well is 60 m south, at $(0,-60)$; the image (recharge) well sits 400 m west, at $(-400,0)$:
$$r_{\text{real}}=60\ \text{m},\qquad r_{\text{image}}=\sqrt{400^2+60^2}=\boxed{404.5\ \text{m}}.$$
Superposition at $t=24$ h. Computing $u=r^2S/4Tt$ and $W(u)$ separately for each well and subtracting (image well is a recharge well, so it partially offsets the real well's drawdown):
$$s(24\text{h})=\frac{Q}{4\pi T}\Big[W(u_{\text{real}})-W(u_{\text{image}})\Big]=\boxed{9.52\ \text{m}}.$$
Superposition at $t=36$ h. Repeating with $t=129{,}600$ s (both $u$-values scale down, both $W$-values increase, but the real well's term still dominates):
$$s(36\text{h})=\boxed{10.15\ \text{m}}.$$
Drawdown continues to grow between 24 and 36 hours (the river boundary limits, but does not fully arrest, the cone of depression's expansion at this distance).
Part (b) — impermeable boundary, obs. well 200 m south, $t=36$ h. Now $r_{\text{real}}=200$ m and $r_{\text{image}}=\sqrt{400^2+200^2}=447.2$ m, and because the image well is also a PUMPING well (no-flow boundary reflects rather than cancels), the two drawdowns ADD:
$$s=\frac{Q}{4\pi T}\Big[W(u_{\text{real}})+W(u_{\text{image}})\Big]=\boxed{5.60\ \text{m}}.$$
Physically, the impermeable boundary forces all of the pumped water to be drawn from the aquifer on the well's own side, which is why the image well reinforces rather than offsets the real well's drawdown.
Figure 4a — River (constant-head) boundary: an image RECHARGE well beyond the boundary offsets the real well's drawdown at the observation well.
Figure 4b — Impermeable boundary: an image PUMPING well reinforces (adds to) the real well's drawdown instead.